Optics



Flat Top, Ultra-Narrow Band Pass Optical Filters Using Plasma Deposited Hard Oxide Coatings Alluxa Engineering Staff September 2012 100

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

Transmission (%)

10

1 cav 2 cav 3 cav 0.1

4 cav 5 cav

0.01

0.001 635

636

637

638

639

640

641

Wavelength (nm)

1

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

1

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

642

643

644

645

Optics



Thin film optical filters with ultra-narrow bandwidth, high transmission and flat spectral profiles improve optical system performance for a variety of applications such as LIDAR, laser cleanup, and instrumentation. Alluxa’s new class of ultra-narrow filters are designed for applications such as laser clean up, LIDAR, telecommunications and instrumentation and offer the narrowest and “squarest” filter profiles in the visible and NIR as well as transmission levels that approach 100%. They are manufactured with Alluxa’s proprietary advanced plasma enhanced PVD process using durable, hard metal-oxide, front surface thin films and are virtually impervious to environmental effects.

Basic Bandpass Theory The design principles of resonant cavity thin film optical bandpass filters are well known and rely on stacked Fabry-Perot resonant cavities. Fabry-Perot resonant thin film optical cavities are a pair of dielectric reflectors separated by a spacer layer of a halfwave thickness or a multiple halfwave of optical thickness. A cavity can be between 3 and 50 layers depending on bandwidth. An excellent book describing the subject further is “Thin Film Optical Filters” by Dr. Angus Macleod. Designing filters to have improved squareness , or steeper slopes, is a relatively simple matter of adding more cavities to the filter design as shown in figure 1 below. To make a filter narrower or wider, the designer increases or decreases the thickness of the spacer layer or increases or decreases the reflectivity of the dielectric mirrors. 100

Transmission (%)

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

10

1 cav 2 cav 3 cav 0.1

4 cav 5 cav

0.01

0.001 635

636

637

638

639

640

641

642

643

644

645

Wavelength (nm)

Fig. 1. Filter squareness is a direct function of number of cavities count.

2

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

1

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

Optics



Adding cavities challenges the deposition process control system, and invariably introduces undesirable ripple and loss to the passband. Alluxa has created a new low noise monitoring system that provides the utmost in layer thickness accuracy, which enables cavities to be added almost without limit. The novel, advanced computer control system constantly measures the filter function and compensates for thickness errors associated with prior layers. The system produces filters with remarkably low ripple and steep slopes that consistently match theory.

The “Ultra” Class of Flat Top Narrow Band Filters Flat top, ultra-narrow hard coated bandpass filters were pioneered by the telecommunications industry in the 1990s and achieved amazingly narrow and high performance results. The narrowest published result was “25 GHz thin film optical filter” presented at OFC in 2002 by Scobey and Fortenberry and demonstrated a bandwidth of .1nm at 1550nm. Filters this narrow suffered however from severe phase delay effects (chromatic dispersion) across the passband due to the high resonant lifetime and were not useful for real world telecommunication systems. These filters were also very small, on the order of a few mm in size, and so limited in usefulness to instrumentation designers. Narrow band filters in the visible region with useful diameters of 25mm to 50mm or larger have been traditionally limited to between 2 and 5 nm in bandwidth due to control system limitations, optical loss and uniformity problems. Alluxa has developed a new class of ultra-narrow bandpass filters that solve these manufacturing issues and can produce bandwidths of less than 1nm in the visible and near IR with flat top and square filters shapes. The measured result of a fully blocked 532 bandpass filter is shown in Fig. 2 below. Note that measuring filters this narrow require special spectrophotometer setups. See Alluxa’s related paper available for download on the Alluxa.com website “Spectrophotometer Measurements for Optical Filters” for discussion of this topic. 100 90 80

Transmission (%)

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

70

50 40

30 20

10 0 530

530.5

531

531.5

532

532.5

533

533.5

534

Wavelength (nm)

Fig. 2 Measured Transmission of a fully blocked 3 cavity flat top bandpass filter at 532nm with 0.92nm bandwidth and T>92%.

3

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

60

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

Optics



Large Formats The bulk of narrowband applications use filters in the 12.5mm to 50mm in diameter. By carefully controlling uniformity of physical and optical thickness, Alluxa has for the first time produced flat top ultra-narrowband filters economically priced in formats up to 250mm. Fig. 3 shows the measured result of various radii of a 250mm flat top bandpass on a 250mm wafer designed to transmit the 532nm laser line. 100 90 80

Transmission (%)

70 60

1 inch 2 Inch

50

3 inch 3.5 Inch

40

4 inch 4.5 Inch

30 20

10 0 530

530.5

531

531.5

532

532.5

533

533.5

534

Wavelength (nm)

Fig. 3 Measured results of 250mm diameter, fully blocked 3 cavity flat top bandpass filter with 0.94nm bandwidth with T>90%.

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

Shift with Angle The filter function of a thin film filter constructed of resonant cavities shifts as it is tilted away from normal to shorter wavelengths. The shape itself stays much the same until relatively high angles where polarization effects begin to become a factor. It is well known that this relative shift in wavelength changes proportionally to the square of the angle of tilt, for tilts up to a few tens of degrees. The proportionality constant is the inverse of the square of the effective index times two, where the effective index is a property of the cavities design as well as the coating materials used. This effect is illustrated in the angle measurements of the narrowband filter shown in Fig. 4. The user needs to take the angle shift effect into consideration when determining the Field of View (FOV) requirements of the filter. For larger FOV applications, the filter bandwidth may need to be increased.

4

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

Optics



100 90 80

Transmission (%)

70 60 0 degrees 3 degrees

50

5 degrees 7 degrees

40

9 degrees 30 20 10 0 529

529.5

530

530.5

531 531.5 Wavelength (nm)

532

532.5

533

533.5

Fig. 4 Shift in wavelength with angle of incidence for a measured laser line filter at 532 nm.

Blocking Performance

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

Alluxa’s ultra-narrow filters can be coupled with additional filtering structures to create wide and deep blocking performance at state of the art levels (up to and beyond OD6) without sacrificing transmission performance. Typical performance specifications are a 400 nm to 1100 nm range around the passband with OD4, OD5, or OD6 blocking performance. Blocking levels typically do not have an impact on transmission, but it can add to the cost of manufacture of the filter.

Optimizing Performance and Cost The wide variety of filter performance requirements that can be designed into Alluxa’s ultranarrow bandpass filters offer the opportunity for optimal performance / cost balance in the finished filter. The most fertile areas for considering performance / cost tradeoff are: blocking range and level, substrate material, and spectral tolerances on filter attributes such as center wavelength (CWL) and full width – half maximum (FWHM), and size and clear aperture.

5

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

Optics



While the blocking requirements do not meaningfully affect the transmission levels achieved in Alluxa’s filters, it does add cost and complexity to the design and coating process due to the additional layers required. In many cases, the cost of the filter may be optimized by carefully addressing the exact blocking range required. In laser cleanup situations, only the ASE spectrum of the laser may need to be blocked to high levels. Alternatively, in a detection application, the blocking requirements will be different depending on whether or not the system is using a PMT, Silicon detector or otherwise. Factoring in the responsivity of the detector can further reduce the layer count in the filter and, therefore, the cost. In terms of substrate material, Alluxa filters are usually coated on either UV grade fused silica or Borofloat 33 in varying sizes and thicknesses. In most applications, Borofloat 33 offers a sufficiently high quality, durable optical glass. In some cases, the use of fused silica is necessary – particularly in applications where there is extreme sensitivity to auto-fluorescence of the substrate material. When considering the spectral profile of ultra-narrow filters, additional constraints on the filter shape such as CWL and FHWM tolerances can have significant impact on cost. The simplest method for specification of the spectral profile is to call for an absolute transmission at a defined wavelength and to call for the bandwidth to be less than a defined spacing. The filter in the figure above was specified in this way: > 92% Transmission at 532 nm and < 1 nm FWHM. Any additional tolerances to define the spectral shape should be considered in terms of their value to the application as the effect on cost can be large.

Summary Flat top and square narrowband filters of less than 1nm in bandwidth and transmission of >90% even 95% are now available at sizes of up to 250mm in diameter. Out of band blocking levels of 3 OD to 6OD can easily be added. These filters can be used for a wide range of applications such as LIDAR, laser based remote sensing, laser clean up, telecommunications and other instrumentation applications.

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

Glossary Angle of Incidence (AOI): The angle at which a filter is tilted relative to the primary ray. For example, an AOI of 0 means the primary ray is perpendicular to the plane of the filter. Bandpass Filter: A filter that transmits a band of wavelengths while blocking the wavelengths on either side of the passband. Blocking: The level of rejection of light outside the passband.

6

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

Optics



Center Wavelength (CWL): The center of the passband for a bandpass filter. Another common definition is the average of the 50% of peak of each edge of a bandpass filter. Cone Angle: The range of angles of light incident on the filter about the AOI. Cone Angle Average: Average of transmission or reflection across the cone angle Dichroic: A filter that transmits one band and reflects a different band Edge Filter: A filter that transmits a band of wavelengths and blocks only low side (long wave pass) or high side (shortwave pass) of wavelengths. Fused Silica: Substrate material composed of amorphous silicon dioxide. Long Wave Pass (LWP): An edge-type filter that transmits longer wavelengths and blocks shorter wavelengths. Notch Filter: A filter that blocks a narrow range while transmitting wavelengths on either side of the blocked wavelength range. Optical Density (OD): The log (base 10) of transmittance (T). (T on a zero to unity scale) Passband: The range of wavelengths that are desired to be transmitted. Ripple: Variations in transmission in the passband. Shortwave Pass (SWP): An edge-type filter that transmits the shorter wavelengths and blocks higher wavelengths. Spectral Slope: Rate of change of the spectrum from a passband to a blocking band.

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

Transmitted Wavefront Error (TWE): Distortion of the wavefront of a plane wave as it transmits through a filter, generally given in units of the HeNe wavelength of 633nm.

Alluxa

Alluxa designs and manufactures next generation hard coated optical filters using a proprietary plasma deposition process in Santa Rosa, CA. Alluxa’s unique, purpose-built deposition platform and control systems were designed, developed, and built by our team in Santa Rosa, CA to address the demanding requirements of the next generation of systems and

7

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk

Optics



instruments. This unique technology allows Alluxa to create the world’s most challenging filters at breakthrough price points. Contact Alluxa for more information at [email protected] or visit our website at http://www.alluxa.com

11/16 / V02 / HW / alluxa/ultra-narrow-bandpass-filter

All content copyright ©2012 Alluxa

8

Germany & Other Countries Laser Components GmbH Tel: +49 8142 2864 – 0 Fax: +49 8142 2864 – 11 [email protected] www.lasercomponents.com

United Kingdom Laser Components (UK) Ltd. Tel: +44 1245 491 499 Fax: +44 1245 491 801 [email protected] www.lasercomponents.co.uk